The applied method provides plausible values for the coronal
Alfvén velocity and magnetic field. The data scatter is much
larger than the errors of measurement thus indicating a diversity
of densities and field strengths in the corona. The magnetic field
strength decreases from 1-7 G at
to 0.3-0.9 G at
.
Such a result is in a good agreement with
other estimates at this height range, as well as with the
B=5H-1.5 relationship proposed by
Dulk & McLean (1978). When placed in the wider context together with the
data covering the 1<R<10 range, the data indicate that below the
height of
the magnetic field is governed by the
active region fields. Above
the radial field,
decreasing as R-2, becomes dominant.
The results show that the coronal value of the parameter is around
,
slowly increasing with the height.
This is consistent with the generally decreasing trend of the
Alfvén velocity (Fig. 3a) since the coronal temperature
can be considered as approximately constant. Beside the overall
decreasing trend, the data indicate that there is a local minimum
of the Alfvén velocity of
400-500 km s-1at
1.7-2.2 and a local maximum of
450-700 km s-1 at
1.8-2.5,
depending on the coronal density model used. Such behaviour of the
Alfvén velocity is qualitatively similar to that anticipated by
Mann et al. (2002).
The inferred shock velocities decrease, whereas the density jumps
increase in the region of
.
Most of the dm-m type II
bursts start at heights lower or close to the Alfvén velocity
minimum and cease close to the heights where it attains the
maximum.
Finally, we note that the frequency drift of dm-m type II bursts
depends on the emission frequency as a power-law
,
very similar to that found by Vrsnak et al. (2001b) in IP type II bursts.
Acknowledgements
We are grateful to the Culgoora Solar Observatory for the open data policy. We are thankful to Dr. P. Zlobec for helpful comments and suggestions. J.M. acknowledges a grant under MIUR Cofin.
Copyright ESO 2002